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AD8626ARM-R2 数据表(PDF) 15 Page - Analog Devices |
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AD8626ARM-R2 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() AD8627/AD8626/AD8625 Rev. B | Page 15 of 20 MINIMIZING INPUT CURRENT The AD862x is guaranteed to 1 pA max input current with a ±13 V supply voltage at room temperature. Careful attention to how the amplifier is used will maintain or possibly better this performance. The amplifier’s operating temperature should be kept as low as possible. Like other JFET input amplifiers, the AD862x’s input current doubles for every 10°C rise in junction temperature, as illustrated in Figure 8. On-chip power dissipation raises the device operating temperature, causing an increase in input current. Reducing supply voltage to cut power dissipation reduces the AD862x’s input current. Heavy output loads can also increase chip temperature; maintaining a minimum load resistance of 1 kΩ is recommended. The AD862x is designed for mounting on PC boards. Maintaining picoampere resolution in those environments requires a lot of care. Both the board and the amplifier’s package have finite resistance. Voltage differences between the input pins and other pins as well as PC board metal traces may cause parasitic currents larger than the AD862x’s input current, unless special precautions are taken. For proper board layout to ensure the best result, refer to the ADI website for proper layout seminar material. Two common methods of minimizing parasitic leakages that should be used are guarding of the input lines and maintaining adequate insulation resistance. Contaminants such as solder flux on the board’s surface and the amplifier’s package can greatly reduce the insulation resistance between the input pin and traces with supply or signal voltages. Both the package and the board must be kept clean and dry. PHOTODIODE PREAMPLIFIER APPLICATION The low input current and offset voltage levels of the AD862x, together with its low voltage noise, make this amplifier an excellent choice for preamplifiers used in sensitive photodiode applications. In a typical photovoltaic preamp circuit, shown in Figure 45, the output of the amplifier is equal to (P)Rf R ID(Rf) V p OUT − = − = where: ID = photodiode signal current (A) Rp = photodiode sensitivity (A/W) Rf = value of the feedback resistor, in Ω P = light power incident to photodiode surface, in W The amplifier’s input current, IB, contributes an output voltage error proportional to the value of the feedback resistor. The offset voltage error, VOS, causes a small current error due to the photodiode’s finite shunt resistance, RD. The resulting output voltage error, VE, is equal to ) Rf(I V R R V B OS D f E + ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ + = 1 A shunt resistance on the order of 100 MΩ is typical for a small photodiode. Resistance RD is a junction resistance that typically drops by a factor of two for every 10°C rise in temperature. In the AD862x, both the offset voltage and drift are low, which helps minimize these errors. With IB values of 1 pA and VOS of 50 mV, VE for Figure 45 is very negligible. Also, the circuit in Figure 45 results in an SNR value of 95 dB for a signal bandwidth of 30 kHz. RD 100M Ω C4 15pF IB IB VOS CF 5pF RF 1.5M Ω OUTPUT AD8627 PHOTODIODE Figure 45. A Photodiode Model Showing DC Error OUTPUT AMPLIFIER FOR DIGITAL-TO-ANALOG CONVERTERS Many system designers use amplifiers as buffers on the output of amplifiers to increase the DAC’s output driving capability. The high resolution current output DACs need high precision amplifiers on their output as current to voltage converters (I/V). Additionally, many DACs operate with a single supply of 5 V. In a single-supply application, selection of a suitable op amp may be more difficult because the output swing of the amplifier does not usually include the negative rail, in this case AGND. This can result in some degradation of the DAC’s specified perform- ance unless the application does not use codes near zero. The selected op amp needs to have very low offset voltage—for a 14-bit DAC, the DAC LSB is 300 µV with a 5 V reference—to eliminate the need for output offset trims. Input bias current should also be very low because the bias current multiplied by the DAC output impedance (about 10 kΩ in some cases) adds to the zero code error. Rail-to-rail input and output performance is desired. For fast settling, the slew rate of the op amp should not impede the settling time of the DAC. Output impedance of the DAC is constant and code independent, but in order to minimize gain errors, the input impedance of the output amplifier should be as high as possible. The AD862x, with very high input impedance, IB of 1 pA, and fast slew rate, is an ideal amplifier for these types of applications. A typical configuration with a popular DAC is shown in Figure 46. In these situations, the amplifier adds another time constant to the system, increasing the settling time of the output. The AD862x, with 5 MHz of BW, helps in achieving a faster effective settling time of the combined DAC and amplifier. |
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